Electric field of a point charge

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A point charge is a theoretical concept representing an infinitely small charge, often described using a Dirac delta function for charge density. It is not limited to an electron but can represent any charge concentrated at a single point in space. The discussion emphasizes that this model recovers Coulomb's law through mathematical integration and application of Gauss' law. When applying the divergence theorem, the relationship between electric field and charge density is established, leading to the familiar expression for the electric field around a point charge. Ultimately, the point charge serves as a simplified model for understanding electric fields in physics.
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I am trying to understand what a point charge is.
I am trying to understand what a point charge is. Is it just an electron? Or is it just an idea?
 
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A point charge ##q## at position ##\vec{r}_0## is described by a charge density consisting of a Dirac delta function, ##\rho(\vec{r}) = q\delta^{3}(\vec{r} - \vec{r}_0)##.

Edit: N.B. you can also check that this recovers the Coulomb law, i.e. from Maxwell I,$$\nabla \cdot \vec{E} = \frac{\rho}{\varepsilon_0}$$Perform a volume integral over a region ##\Omega## on both sides, and then use the divergence theorem on the LHS,$$\int_{\partial \Omega} \vec{E} \cdot d\vec{S} = \frac{1}{\varepsilon_0} \int_{\Omega} q\delta^3(\vec{r} - \vec{r}_0) dV = \frac{q}{\varepsilon_0}$$That's Gauss' law in integral form, which you can convert to Coulomb's law by choosing ##\partial \Omega## to be a spherical surface concentric with the point charge, of radius ##R##, $$4\pi R^2 E_r = \frac{q}{\varepsilon_0} \implies E_r = \frac{q}{4\pi \varepsilon_0 R^2}$$
 
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It's just a theoretical concept. It's infinitely small. There's not much more than that to it. And yes, if you want to describe it as a charge distribution you'd use a three dimensional dirac delta function for it.
 
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